Methods, Systems and Apparatuses for Optically Addressed Holographic Imaging System

ABSTRACT

Methods and systems and components made according to the methods and systems, are disclosed relating to the generation of a holographic image, including a color-containing holographic image, generated exclusively optically addressing information to a projection system.

This application is a divisional of prior U.S. patent application Ser.No. 15/083,589, filed 29 Mar. 2016, the disclosure of which isincorporated by reference herein in its entirety.

TECHNOLOGICAL FIELD

The present disclosure generally relates to the field of image display.More particularly, the present disclosure relates to the field ofaddressed light, particularly optically addressed light for the purposeimproving holographic imaging displays, apparatuses, systems andmethods.

BACKGROUND

Images are typically created on a display by electrically addressinglight, for example via a spatial light modulator, images are created andchanged electronically and projected onto electronic displays. A spatiallight modulator (SLM) is an object that imposes some form of spatiallyvarying modulation on a beam of light. Usually a SLM modulates theintensity of the light beam, although devices are known that modulatethe phase of the beam or both the intensity and the phasesimultaneously. Nevertheless, known imaging devices rely onelectronically addressing inputs. Such electrically addressed inputsrealize practical limitations relative to scale. That is, for example,known electrically addressed imaging systems must use projection meansof a certain minimum size or otherwise realize various systemconstraints relative to image delivery and performance. This inabilityto miniaturize imaging systems has restricted the advancement of imagingdevices relative not only to size, but also in terms of intensity,resolution, color, etc.

In addition, the technology relating to the projection of realisticholograms to date has been cumbersome and not entirely useful orreliable. While so-called optically addressed imaging systems are knownusing optically addressable electrophoretic displays, or opticallyaddressed spatial light modulation, such imaging systems alsoincorporate electrical components that, again, place scale, quality andother restrictions on the overall imaging system.

BRIEF SUMMARY

The present disclosure relates to methods, systems and apparatuses forexclusively addressing electronic media optically.

According to one aspect, a method is disclosed for addressing aprojection system comprising: positioning an electro-optical device forinputting information to a projection system; applying a voltage acrossthe projection system device, with the voltage generated byvoltage-generating device; generating plasma in a plasma-containingdevice; generating a plurality of write beam frequencies from theelectro-optical device; directing the write beam frequencies to interactwith the plasma in the plasma-containing device; generating a pluralityof write beams with each write beam having a phase value, with eachphase value being different; generating a coherent read beam from acoherent read beam-generating source; controlling the write beamfrequencies independently from the read beam; generating predeterminedphase values; and generating a holographic image, wherein the writebeams are exclusively optically addressed from the electro-opticaldevice to the plasma-containing device.

In a further aspect, information is exclusively optically addressed tothe plasma-containing device via the write beams.

Another aspect is directed to a holographic image generated byexclusively optically addressing information from an electro-opticaldevice to a projection system comprising a plasma-containing device.

In another aspect, the electro-optical device is a laser and the writebeams are emitted from the laser.

Another aspect further comprises, coincidently with the step ofgenerating a holographic image, the step of assigning color to theholographic image by modulating the different write beam frequencies inphase separately in the wavefront.

In yet another aspect, the holographic image comprises a plurality ofcolors.

A further aspect of the present disclosure is directed to a projectionsystem comprising, the projection system comprising: an electro-opticaldevice configured to input information to a plasma-containing device; avoltage-generating source in communication with the plasma-containingdevice; a plurality of write beam frequencies generated by theelectro-optical device, with the plurality of write beam frequencieseach configured to interact with the plasma-containing device togenerate a plurality of write beams having a plurality of phase values,with each phase value being different from one another; a coherent readbeam generated from a coherent read beam source; a first controllerconfigured to control the phase values to produce predetermined phasevalues in a phase modulated beam; a second controller configured tocontrol the write beam, the second controller configured to operateindependently from the first controller; wherein the information isconfigured to be generated exclusively optically from theelectro-optical device to the plasma-containing device, and theexclusively optically addressed information is configured to generate aholographic image.

In a further aspect, information is exclusively optically addressed tothe projection system device via the write beams.

In another aspect, the electro-optical device is a laser and the writebeams are emitted from the laser.

In a further aspect, exclusively optically addressed information isconfigured to assign at least one color to the holographic image.

Yet another aspect is directed to an object comprising a projectionsystem comprising: an electro-optical device configured to inputinformation to a projection system, with the projection systemcomprising a plasma-containing device; a voltage-generating source incommunication with the plasma-containing device; a plurality of writebeam frequencies generated by the electro-optical device, with theplurality of write beam frequencies each configured to interact withplasma in the plasma-containing device to create a plurality of writebeams having a plurality of phase values, with each phase value beingdifferent from one another; a coherent read beam produced by a coherentread beam source; a first controller configured to control the phasevalues to produce predetermined phase values; a second controllerconfigured to control the write beam, the second controller configuredto operate independently from the first controller; wherein theinformation is configured to be exclusively optically addressed from theelectro-optical device to the plasma-containing device, and theoptically generated information is configured to generate a holographicimage.

In yet another aspect, a stationary object comprises the exclusivelyoptically addressable projection system comprising an electro-opticaldevice configured to exclusively optically address information to aprojection system.

In another aspect, a vehicle comprises the optically addressableprojection system comprising an electro-optical device for exclusivelyoptically addressing information to a projection system.

In further aspects, vehicles that comprise an exclusively opticallyaddressable projection system comprising an electro-optical device forinputting information to a projection system include: a manned aircraft,an unmanned aircraft, a manned spacecraft, an unmanned spacecraft, amanned rotorcraft, an unmanned rotorcraft, a manned satellite, anunmanned satellite, a rocket, a manned terrestrial vehicle, an unmannedterrestrial vehicle, a manned surface water borne vehicle, an unmannedsurface water borne vehicle, an unmanned sub-surface water bornevehicle, a manned sub-surface water borne vehicle or combinationsthereof.

According to a further aspect, a method is disclosed for addressing aprojection system comprising: positioning an electro-optical device forinputting information to a projection system, with the projection systemcomprising a solid state device; applying a voltage generated by avoltage-generating device across the solid state device, generating aplurality of write beam frequencies from the electro-optical device;directing the write beam frequencies to interact with the solid statedevice; generating a plurality of write beams with each write beamhaving a phase value, with each phase value being different from oneanother; generating a coherent read beam from a coherent readbeam-generating source; controlling write beams independently from theread beam; generating predetermined phase values; and generating aholographic image, wherein the write beams are exclusively opticallyaddressed from the electro-optical device to the solid state device.

In a further aspect, information is exclusively optically addressed tothe solid state device via the write beams.

Another aspect is directed to a holographic image generated byexclusively optically addressing information from an electro-opticaldevice to a projection system comprising a solid state device.

In another aspect, the electro-optical device is a laser and the writebeams are emitted from the laser.

Another aspect further comprises, coincidently with the step ofgenerating a holographic image, the step of assigning color to theholographic image by modulating the different write beam frequencies inphase separately in the wavefront.

In yet another aspect, the holographic image comprises a plurality ofcolors.

In yet another aspect, the solid state device comprises a semiconductormaterial.

Yet another aspect is directed to an object comprising a projectionsystem comprising: an electro-optical device configured to inputinformation to a projection system, with the projection systemcomprising a solid state device; a voltage-generating source incommunication with the solid state device; a plurality of write beamfrequencies generated by the electro-optical device, with the pluralityof write beam frequencies each configured to interact with the solidstate device to create a plurality of write beams having a plurality ofphase values, with each phase value being different from one another; acoherent read beam produced by a coherent read beam source; a firstcontroller configured to control the phase values to producepredetermined phase values in a phase modulated beam; a secondcontroller configured to control the write beam, the second controllerconfigured to operate independently from the first controller; whereinthe information is configured to be addressed exclusively optically fromthe electro-optical device to the solid state device, and the opticallygenerated information is configured to generate a holographic image.

In yet another aspect, a stationary object comprises the exclusivelyoptically addressable projection system comprising an electro-opticaldevice configured to exclusively optically address information to aprojection system.

In another aspect, a vehicle comprises the optically addressableprojection system comprising an electro-optical device for exclusivelyoptically addressing information to a projection system.

In further aspects, vehicles that comprise an exclusively opticallyaddressable projection system comprising an electro-optical device forinputting information to a projection system include: a manned aircraft,an unmanned aircraft, a manned spacecraft, an unmanned spacecraft, amanned rotorcraft, an unmanned rotorcraft, a manned satellite, anunmanned satellite, a rocket, a manned terrestrial vehicle, an unmannedterrestrial vehicle, a manned surface water borne vehicle, an unmannedsurface water borne vehicle, an unmanned sub-surface water bornevehicle, a manned sub-surface water borne vehicle or combinationsthereof.

In yet another aspect, a stationary object comprises an exclusivelyoptically addressable projection system comprising an electro-opticaldevice for exclusively optically addressing information to a projectionsystem.

In another aspect, a vehicle comprises the optically addressableprojection system comprising an electro-optical device for exclusivelyoptically addressing information to a projection system.

In further aspects, vehicles that comprise an exclusively opticallyaddressable projection system comprising an electro-optical device forinputting information to a projection system comprise: a mannedaircraft, an unmanned aircraft, a manned spacecraft, an unmannedspacecraft, a manned rotorcraft, an unmanned rotorcraft, a mannedsatellite, an unmanned satellite, a rocket, a manned terrestrialvehicle, an unmanned terrestrial vehicle, a manned surface and/orsub-surface water borne vehicle, an unmanned surface and/or sub-surfacewater borne vehicle or combinations thereof.

In a further aspect, the present disclosure is directed to a method foraddressing a projection system comprising: positioning anelectro-optical device for optically addressing a projection system;with the projection system comprising a solid state device; applying avoltage-generating source in communication with the solid state device;generating a write beam in the electro-optical device; directing thewrite beam to a predetermined location in the solid state device; andgenerating a pixelated output in the solid state device, with theoptically generated information configured to generate a holographicimage, and with the holographic image comprising predetermined colors.

In another aspect, the present disclosure is directed to a projectionsystem comprising an electro-optical device configured to produce awrite beam and optically address a projection system output, with theprojection system output comprising a solid state device; and avoltage-generating source in communication with the solid state device,wherein the input information is configured to generate photonicexcitation at predetermined pixel locations in the solid state device,with optically generated information configured to generate aholographic image, and with the holographic image comprisingpredetermined colors.

BRIEF DESCRIPTION OF THE DRAWINGS

Having thus described variations of the disclosure in general terms,reference will now be made to the accompanying drawings, which are notnecessarily drawn to scale, and wherein:

FIG. 1 is schematic diagram of an Prior Art device showing electricallyaddressing an imaging display;

FIGS. 2 and 3 are schematic diagrams showing an aspect of the presentdisclosure where a plasma-containing projection device is exclusivelyoptically addressed;

FIGS. 4A and 4B are schematic diagrams showing an aspect of the presentdisclosure where a plasma-containing projection device (FIG. 4A) and asolid state-containing projection device (FIG. 4B) are exclusivelyoptically addressed and generate phase modulated beams to generate aholographic image;

FIGS. 5 and 6 are flow charts according to aspects of the presentdisclosure; and

FIG. 7 is a drawing of an aircraft comprising a cockpit section havingvarious display devices.

DETAILED DESCRIPTION

An imaging system that is completely optically addressed wouldsignificantly improve imaging system flexibility including, but notlimited to, image contrast, image quality, image presentation, imageaccuracy/reproducibility, image variation color selection, imageintensity, image resolution (e.g. sharpness), image projection devicescale and image projection display scale, reduction in devicecomplexity, etc.

Aspects of this disclosure are directed to projection or image-producingmethods, systems and apparatuses, including architecture for addressinga plasma-based or solid-state-based projection or image-producing systemin an all optical, or exclusively optical fashion. The term “addressing”means that the information input to, and output from the display (plasmatube or solid-state device) is completely and exclusively optical (e.g.electromagnetic radiation) in its physical nature. Such exclusivelyoptical addressing is significantly distinct from the known systemswhere information for image projection and display is providedelectronically, with an optical output only. According to aspects of thepresent disclosure, “optically addressed” information is delivered to adisplay (e.g. projector, etc.) exclusively optically, and suchinformation is not delivered to a display electrically, as is presentlythe case with typical display systems.

According to further aspects of the present disclosure, an optical beam,such as, for example, one emitted from a laser, is understood to be awell-defined beam in its propagation characteristics; (e.g. an opticalbeam having a well-defined wavefront, and well-defined spectralcharacteristics). While the spectrum does not have to be narrow, theuseful spectral characteristics are understood to be substantiallyconstant. While beams emitted from laser sources satisfy the abovecriteria, non-laser (e.g. non-coherent) sources that satisfy the abovecriteria are also contemplated according to aspects of the presentdisclosure.

For example, FIG. 1 shows a schematic representation of a Prior Artprojection system 10 showing a device that is electrically addressed. InFIG. 1, a plasma tube 12 is shown in a side view. The volume of thistube contains a gas 14. Such gas 14 has a voltage 16 placed across it.The voltage dissociates enough for electrons from the gas to enable thetube contents to behave as a plasma. In order to generate the individualpixels for projecting an image, individual electrical elements 17 areattached to the back side 12 a of the plasma tube 12. While shown as asingle row, it is understood such electrical elements may be dispersedin two dimensions (e.g. also perpendicular to the drawing sheet). Theelectrical elements 17, acting individually, both for position andcolor, have voltages applied to them. When the voltages are sufficientto dissociate electrons from the gas, the associated electric field willcreate a current through the plasma, generating a light signal (e.g. theprojected image that is emitted from the front side 12 b of the plasmatube 12) represented in FIG. 1 as arrows pointing to the left. In thisformat as shown in FIG. 1 and described above, the plasma tube 12 issaid to be “electronically addressed” in the sense that the informationconcerning the desired image is carried electrically to the plasma tube.

FIG. 2 is a schematic representation of an exclusively opticallyaddressed projection system 20 according to aspects of the presentdisclosure. In FIG. 2 a plasma tube 22 is shown in a side view having avoltage from a voltage generating source 24 applied across the plasmatube 22. The voltage is applied across the plasma tube 22 to provide asufficiently large electric field in the plasma tube 22 to generate aplasma. According to the projection system 20, plasma tube 22 comprisesa front reflective surface 22 a and a back reflective surface 22 b. Thereflectivities of the surfaces 22 a and 22 b are based on the desiredapplication and system. However, generally, the reflectivities of thesurfaces 22 a and 22 b are greater than about 90%, and ranging fromabout 90% to about 99.9%, and more preferably for aspects of the presentdisclosure from about 90% to about 95%. According to aspects of thepresent disclosure, if the front and back reflective surfaces of theplasma tube 22 are optically flat and substantially parallel to oneanother, the plasma tube with surfaces 22 a and 22 b will behave like aFabry-Perot interferometer, with a reflected optical pattern generatedby interference between the front and back surfaces of the plasma tube22. It is understood that the optical path length associated with theinterference depends upon the index of refraction, “n”, of the plasmacontained within the plasma tube 22. R₁ and R₂ refer to the reflectivityvalues of the front and back surfaces of the plasma-containing devicerespectively. The values are preferably identical or close to identicalto achieve optimal performance. However, the “R” values of the front andback surfaces may vary by up to about 5% from one another. According tothis aspect of the present disclosure, a “write” beam 26 is directedfrom a write beam source 25 to a frequency selective beamsplitter 27that reflects only a predetermined frequency of the write beam 26. Thepredetermined frequency is selected to be a frequency that can be easilyabsorbed by the plasma in the plasma-containing device. The frequencydepends upon the material present in the plasma. Preferred frequenciesaccording to the present disclosure are typically in the infrared range(e.g. 3 μm or longer) or in the ultraviolet range (e.g. 300 nm orshorter). The infrared values substantially coincide with vibrationalexcitations in the plasma while the ultraviolet values coincide withelectronic excitations. The write beam 26 is created to be “on” or “off”(light or no light) at each x-y position within the cross-section of thewrite beam 26, depending on the image that needs to be projected. If thewrite beam 26 is at a frequency where the plasma is strongly absorptive(e.g. in the UV range) the absorption within the plasma will cause ashift in the value of “n”, but only at the points (e.g. locations) wherethere is light in the write beam 26. In this way, the write beam 26causes a two dimensional modulation in the interference pattern. Thechange in the interference pattern is then used to establish whichplasma pixels will be on and which will be off. As shown in FIG. 2, theprojected light from the plasma then exits the projection system to theleft as emitted light 28. Since the frequency of the emitted light willbe engineered to be lower than the frequency of the write beam 26, itwill pass through the beamsplitter 27. In this way, the plasma tube issaid to be completely and exclusively optically addressed, in that, thepixels for the projected image are created exclusively by theinteraction with the write beam. While there is a voltage present, thevoltage only “conditions” the tube to generate plasma no information isprovided to the system electrically. When the plasma tube is a glasstube, the reflective surfaces of the plasma tube may be added coatingsor coating layers comprising a metal oxide coating, with the reflectivesurfaces also functioning as electrodes for the plasma production in thetube. With regard to particular examples, the reflective surfaces (22 a,22 b) may comprise magnesium oxide, magnesium fluoride, silicon dioxide,tantalum pentoxide, zinc sulfide, titanium dioxide, alone or incombination, etc. Coatings made from these or other materials arecontemplated by aspects of the present disclosure and can be used tocoat the plasma tube, with the coatings producing a reflectivity rangingfrom about 90% to about 99.9%, and more preferably, for certain aspectsof the present disclosure, from about 90% to about 95%. Such MgOcoatings are available from CVI Laser Optics/CVI Melles Griot,Albuquerque, N. Mex. and OCLI (Optical Coatings Laboratory Inc.), SantaRosa, Calif. According to a further aspect, indium tin oxide (ITO) canbe used as a coating for a transparent electrode in theplasma-containing device. The ITO coating has a reflectivity rangingfrom about 4% to about 6% (about 95% transmissivity), and can be used incombination with other coatings to produce a desired reflectivityranging from about 90% to about 95%. Further, when a coating is to bedeposited onto the plasma-containing tubes described herein, accordingto further aspects, the coatings can be deposited onto the tube atthicknesses ranging from about 10 microns to about 100 microns. Theplasma tubes may also be made from a material that is itself inherentlyreflective in the ranges desired.

An illustrative projection system 30 is shown in the schematicrepresentation provided as FIG. 3. A plasma tube 32 has a voltage from avoltage generating source 31 applied across the plasma tube 32comprising back reflective surface 32 a and front reflective surface 32b. However, as with the equivalent reflective surfaces disclosed above22 a, 22 b, generally, the reflectivities of the reflective surfaces 32a and 32 b are greater than about 90%, ranging from about 90% to about95%, and could go as high as 99% subject only to practical operatingparameters of the devices disclosed. Again, according to oneillustrative and non-limiting example, the reflective surfaces (32 a, 32b) comprise magnesium oxide (MgO) having a thickness ranging from about10 microns to about 100 microns. A write beam 36 generated from anelectro-optical device 37 is coupled into the path of the projection, or“read” beam 34 (generated from a projected beam source 35) with afrequency selective beamsplitter 38. Small electronic connections “a”are shown to the left side of the plasma tube 32. The electronicconnections “a” define individual pixels. The write beam 36 modifies thelocal refractive index as stated above. In this variation, however, careis taken to register the information pixels in the write beam with theelectronically connected pixels. The projected image is shownpropagating through the beamsplitter 38 and through the plasma tube 32.The write beams 36 and read beams 34 combine in the plasma tube 32. Asmentioned above, this variation is specific to situations where it isdesirable or necessary to locally control the electric field applied tothe plasma tube. Such flexibility may be needed because a particularimaging application requires a stronger non-linear interaction in onearea than another. As a result, the effect of the write beam on therefractive index of the material in the plasma tube may require enhancednonlinearity. In such cases, local electronic pixilation will increasethe strength of the non-linear interaction, leading to an enhancedeffect on the projected read beam. Such a protocol could also be used tocompensate for inconsistencies within either the write beam or readbeam, thus alleviating the need for additional optics that could berequired to produce a clean wavefront.

In this way, the plasma tube is said to be completely or exclusivelyoptically addressed, in that, the pixels for the projected image arecreated exclusively by the interaction with the write beam. While thereis a voltage present, the voltage only conditions the tube to generateplasma and “condition” the plasma tube and no information is provided tothe system electrically.

Further aspects of the present disclosure are directed to, exclusivelyoptically addressed imaging systems for the improved generation ofthree-dimensional images, including holographic projections, orholograms. Currently known holographic projection schemes are incapableof operating in other than single color modes. In addition, the abilityof known hologram systems to perform in real time or in video formats ispoor. Typical hologram systems are configured with electronic ormechanical systems causing low resolution, low speed of responseresulting in overall images that are poor representatives of reality.

A hologram, or holographic image, is understood to be a photographicrecording of a light field rather than of an image formed by a lens, andit is used to display a fully three-dimensional image of the holographedsubject, which is seen without the aid of intermediate optics. Thehologram itself is not a true “image” and it is usually unintelligiblewhen viewed under diffuse ambient light. A holographic image is anencoding of the light field as an interference pattern of seeminglyrandom variations in the opacity, density, or surface profile of thephotographic medium. When suitably lit, the interference patterndiffracts the light into a reproduction of the original light field andthe objects that were in it appear to still be there, exhibiting visualdepth cues such as parallax and perspective that change realisticallywith any change in the relative position of the observer. For thepurpose of the present disclosure, the terms “hologram”, “holographicimage” and “holographic projection” are equivalent terms and usedinterchangeably.

Aspects of this disclosure contemplate a means for generating athree-dimensional (also known as holographic) projection system in an“all optical fashion”, with information being exclusively opticallyaddressed. In this case, a hologram is also defined as an image whosewavefront is carefully controlled in a predetermined fashion andengineered in two dimensions to produce a three-dimensional image.

Further aspects contemplate the means for generating a steeringmechanism for generating holographic projections. Since a holographicprojection is generated by controlling the local phase within apropagating wavefront, it is understood to control the phase of thewavefront in the x-y plane perpendicular to the propagation direction.Typically, this is done by using an electronic device that producesphase “lags” across the wavefront. As has now been determined, and iscontemplated and described herein, applying an exclusively opticallyaddressed system for imparting information to the projection device,such as, for example, a plasma-containing or solid state device obviatesthe known holographic imaging and holographic image quality issues fromknown holographic systems.

According to aspects of the present disclosure, an optical beamgenerated from an electro-optical source addresses or writes a phasechange within a plasma tube that has an applied electric field orvoltage. The write beam, through non-linear optical interaction, altersthe local imaginary portion of the complex refractive index. Thisinduced change in the refractive index results in a predeterminedmodulation in the local phase of a holographic projection beam that thenforms the holographic image.

Specifically, consider the propagation equations that accompanyelectromagnetic radiation. The form of the plane wave is e^(kx−iω+iϕ).Here, ϕ represents the phase term accompanying the plane wave. Hologramsare coherent projections, in that the phase is well controlled, both inspace and time.

FIGS. 4A and 4B schematically present a three-dimensional projectionsystem 40A, 40B comprising a projection device 32, 42 shown in a sideview. The projection beam, or “read” beam 34 is a coherent light thatcan be described by the plane wave mathematical form as representedabove. The projection beam 34 (emitted from a projection beam source 35)is combined with a write beam 36 addressed from an electro-opticaldevice 37 via a frequency sensitive beamsplitter 38 that reflects thewrite beam frequency while transmitting the projection beam frequencies.A voltage from a voltage source 31 is applied across the projectiondevice. It is understood that the projection device may comprise plasmain a plasma-containing device 32, or the projection device may comprisea solid state device 42 such as, without limitation, semiconductordevices comprising semiconductor materials, etc. The terms “projectionbeam” and “read beam” are equivalent terms for the purposes of thisdisclosure, and such terms are used interchangeably.

In the case of a plasma-containing projection device 40 a, as shown inFIG. 4A, the write beam frequencies will interact with the plasma in theprojection device 32 having a reflective back surface 32 a andreflective front surface 32 b, changing the local (e.g. x-y across thewavefront) values of the refractive index. This will cause slightlydifferent optical path lengths through the plasma tube. As shown in FIG.4, the result will be that the beam wavefront (as represented by thearrows to the left of the plasma-containing device) will each havedifferent phase values. In other words, the values for e^(iϕ) will haveϕ that is dependent upon its position within the wavefront as it travelsto the left, away from the projection device. FIG. 4A shows a projectionsystem of FIG. 3, now with the phase modulated beams 36 a exiting theplasma-containing device 32, wherein the exiting beams converge to apoint in space to form a holographic image (as perceived by a viewer asthe image forms and is focused at the retina of the viewer). Theholographic image, or hologram, can therefore be modulated viaexclusively optically addressed information, with the informationcontaining, for example, desired and predetermined color and colorvariations throughout the holographic image.

The fact that this is a coherent signal (once the ϕ values areestablished, they are constant relative to one another) means that theprojected beam is a hologram. As such, it is capable of displayingobjects in three dimensional representations.

FIG. 4B shows the projection system 40 b, similar is all substantiveways to the projection system 40 a shown in FIG. 40a , with oneexception: the projection device 42 in FIG. 4B is a solid state device,replacing the plasma-containing device 32 of FIG. 4A.

FIGS. 5 and 6 are flowcharts showing various aspect of the presentdisclosure. The following flowcharts disclose methods that may be usedwith various exemplary systems disclosed herein.

FIG. 5 is a flowchart outlining a process 50 according to an aspect ofthe present disclosure, whereby information that is exclusivelyoptically addressed can be implemented to achieve high resolutionthree-dimensional projections, or holograms, including holograms havinga predetermined color, or a plurality of predetermined colors. As shownin FIG. 5, aspects of the present disclosure are directed to a methodfor addressing a projection system 50 to produce holographic imagescomprising positioning an electro-optical device for inputtinginformation to a projection system 51; applying voltage across aplasma-containing device 52; generating plasma in the plasma-containingdevice 53; generating a plurality of write beam frequencies 54;directing the write beam frequencies to interact with plasma in theplasma-containing device 55; generating a plurality of write beams witheach write beam having a distinct and predetermined phase value 56;generating a coherent read beam 57; controlling phase values of writebeams and read beam 58; controlling write beam independently from readbeam 59; and generating a holographic image 60.

Aspects of the present disclosure further contemplate aplasma-containing device being substituted with a solid state device,such as, for example and without limitation, a semiconductor, or othernon-plasma-containing solid state device, etc. As shown in FIG. 6,aspects of the present disclosure are directed to methods for addressinga projection system 70 to produce holographic images comprisingpositioning an electro-optical device for inputting information to aprojection system 71; applying voltage across a solid state device 72;generating a plurality of write beam frequencies 73; directing the writebeam frequencies to the solid state device 74; generating a plurality ofwrite beams with each write beam having a distinct and predeterminedphase value 75; generating a coherent read beam 76; controlling phasevalues of write beams independently from read beam 77; generatingpredetermined phase values 78; and generating a holographic image 79.

The variations and alternatives of the present disclosure relate to themanufacture and use of components and parts such as, for example,composite component parts of any dimension, including the manufactureand use of components and parts in the fabrication of larger parts andstructures. Such devices include, but are not limited to, components andparts designed to be positioned on the exterior or interior ofstationary objects including, without limitation, bridge trusses,support columns, general construction object, etc. Further objectsinclude, without limitation, atmospheric and aerospace vehicles andother objects, and structures designed for use in space or otherupper-atmosphere environments such as, for example, manned or unmannedvehicles and objects, etc. Contemplated objects include, but are notlimited to vehicles such as, for example, aircraft, spacecraft,satellites, rockets, missiles, etc. and therefore include manned andunmanned aircraft, spacecraft, terrestrial, non-terrestrial, and evensurface and sub-surface water-borne vehicles and objects, etc.

Aspects of the present disclosure contemplate achieving exclusivelyoptically addressable holographic images by co-aligning the write andprojection beams that are then combined in an appropriate optic. Theterm “optic” refers to a device that transmits one beam while reflectingthe other, including, without limitation a dielectric film optic. Oncethe beams are combined, they are propagated to the plasma device or thesolid state device. Since the system is optically addressed, there is noneed to “register” the combined beams with any particular location onthe plasma device. The projected beam exits the plasma device and caneither be projected at a screen (with suitable enlargement, if desired)or kept small in dimension for use with a smaller display such as, forexample, a cockpit avionics display.

FIG. 7 is a drawing of an aircraft 80 with enlarged section 82 showingan internal view of a cockpit's instrument displays. As shown in FIG. 7,an aircraft 80 comprises a forward section 82. Section 82 is also shownfrom an interior view to contain a cockpit 84 having multiple locationsfor display components and display locations, with the components andlocations are shown as parts and locations 86, 88, 90, 92, 94, 96, 97,98. While it is understood that a holographic image is perceived toexist as the image is reproduced at the retina of a viewer's eye, andtherefore is not formed in free space, holographic images are shown inFIG. 7 only as an illustration of where such images 100, 102 areperceived to be by a viewer in the cockpit, for example. Indeed,according to aspects of the present disclosure, in an aircraft cockpit,such as that represented generally in FIG. 7, any surface mayincorporate an information display or information display location ableto generate the information necessary to perceive a holographic image,or hologram, including an image display resulting from exclusivelyoptically addressed information. Such displays may be designed to bedisplayed at any desired and predetermined interior or exterior surface,including, without limitation, output displays, windows, opaquesurfaces, etc.

Aspects of the present disclosure contemplate plasma-containing devicesused as display apparatuses. Such devices include, without limitation,plasma-based monitors, partially ionized gas-based systems,gas-discharge-based systems, etc., including support structures such as,for example, glass, etc. and combinations thereof. Further, contemplateduseful structures are transparent at write and projection beamwavelengths.

Further aspects of the present disclosure contemplate write beamsgenerated by electro-optical devices including, but not limited to,coherent sources such as, for example, lasers; partially coherentsources such as, for example light emitting diodes (LEDs); other lightemitting semiconductor materials or other light sources based onAmplified Stimulated Emission, and other non-coherent sources such as,for example incandescent electro-optical sources, fluorescent sources;or thermal-based electro-optical sources, etc., and combinationsthereof.

Read beams contemplated according to aspects of the present disclosuremay be generated by coherent sources including, without limitation,lasers. The coherent read beam sources may be any source that provides afrequency in the visible spectrum (e.g. ranging from about 770 nm to 300nm).

The present disclosure further contemplates voltage-generatingapparatuses to provide the voltages required to generate plasma inplasma-containing devices. Such voltage generating devices include,without limitation, voltage or current based or limited power supplies,as well as any devices capable of generating useful voltages rangingfrom about 100 volts to about 10,000 volts, more particularly rangingfrom about 500 volts to about 1000 volts.

When introducing elements of the present disclosure or exemplary aspectsor embodiment(s) thereof, the articles “a,” “an,” and “the” are intendedto mean that there are one or more of the elements. The terms“comprising,” “including” and “having” are intended to be inclusive andmean that there may be additional elements other than the listedelements. Although this disclosure has been described with respect tospecific embodiments, the details of these embodiments are not to beconstrued as limitations. While the preferred variations andalternatives of the present disclosure have been illustrated anddescribed, it will be appreciated that various changes and substitutionscan be made therein without departing from the spirit and scope of thedisclosure.

What is claimed is:
 1. A method for addressing a projection systemcomprising the steps of: positioning an electro-optical device forinputting information to a projection system device, the projectionsystem device comprising a solid state device; applying a voltagegenerated by a voltage-generating device across the projection systemdevice; generating a write beam having one or more write beamfrequencies from the electro-optical device; directing the write beam tothe solid state device; modifying a phase of local values of an index ofrefraction of the solid state device according to informationexclusively optically addressed by the write beam; generating a coherentread beam from a coherent read beam-generating source; directing theread beam to the solid state device; and generating a holographic imageas the modified phase of local values of the index of refraction of theplasma modulates the local phase of the coherent read beam.
 2. Themethod of claim 1, wherein the information is exclusively opticallyaddressed to the projection system device via the write beam.
 3. Aholographic image generated according to the method of claim
 1. 4. Themethod of claim 1, wherein the electro-optical device is a laser and thewrite beam is emitted from the laser.
 5. The method of claim 1, furthercomprising, coincidently with the step of generating a holographicimage: optically addressing information, the information assigningdifferent colors to the holographic image by separately modulatingdifferent write beam frequencies in phase.
 6. A holographic imagegenerated according to the method of claim
 5. 7. A projection systemcomprising: a projection device comprising a solid state device; anelectro-optical device configured to input information to the projectiondevice-by generating a write beam having one or more write beamfrequencies and exclusively optically addressing information to thesolid state device by modifying a phase of local values of an index ofrefraction of the solid state device; a voltage-generating source incommunication with the solid state device; a coherent read beam sourceconfigured to generate a coherent read beam and direct the coherent readbeam to the projection device; a first controller configured to controlthe write beam; and a second controller configured to control the readbeam, the second controller configured to operate independently from thefirst controller; wherein information is exclusively optically addressedfrom the electro-optical device to the solid state device, with theexclusively optically addressed information configured to generate aholographic image as the modified phase of local values of the index ofrefraction of the solid state device modulates the local phases of thecoherent read beam.
 8. The system of claim 7, wherein theelectro-optical device is a laser and the write beam is emitted from thelaser.
 9. The system of claim 7, wherein exclusively optically addressedinformation is configured to assign color to the holographic image. 10.An object comprising the system of claim
 7. 11. The object of claim 10,wherein the object is a stationary object.
 12. The object of claim 10,wherein the object is a vehicle.
 13. The vehicle of claim 12, whereinthe vehicle is selected from: a manned aircraft; an unmanned aircraft; amanned spacecraft; an unmanned spacecraft; a manned rotorcraft; anunmanned rotorcraft; a manned terrestrial vehicle; an unmannedterrestrial vehicle; a manned surface water borne vehicle; an unmannedwater borne surface vehicle; a manned sub-surface water borne vehicle;an unmanned sub-surface water borne vehicle, and combinations thereof.